1987
DOI: 10.4310/jdg/1214440849
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The Yamabe problem on CR manifolds

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Cited by 282 publications
(328 citation statements)
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“…Indeed, the Cayley transform Ψ c is a biholomorphism between the unit ball in C n+1 and the Siegel domain; when restricted to the respective boundaries it gives a CR equivalence between S 2m−1 minus a point and H n ≃ ∂Ω n+1 (which is the CR equivalent of the stereographic projection of the unit sphere on the Euclidean space), see also section 3 and [48]. Combining Theorem 1.2 with the fractional Sobolev embedding on the Heisenberg group from [26] we obtain the following energy inequality:…”
Section: Equality Is Attained If and Only Ifmentioning
confidence: 98%
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“…Indeed, the Cayley transform Ψ c is a biholomorphism between the unit ball in C n+1 and the Siegel domain; when restricted to the respective boundaries it gives a CR equivalence between S 2m−1 minus a point and H n ≃ ∂Ω n+1 (which is the CR equivalent of the stereographic projection of the unit sphere on the Euclidean space), see also section 3 and [48]. Combining Theorem 1.2 with the fractional Sobolev embedding on the Heisenberg group from [26] we obtain the following energy inequality:…”
Section: Equality Is Attained If and Only Ifmentioning
confidence: 98%
“…Indeed, ifφ = v 2 m−γ ϕ is another defining function for M and v| M = w, which gives a relation between the contact forms aŝ θ = w 2 m−γ θ, then the corresponding operator is given by Pθ γ (·) = w − m+γ m−γ P θ γ (w ·). In particular, for γ = 1, we obtain the CR Yamabe operator of Jerison-Lee [48] …”
Section: Scattering Theory and The Conformal Fractional Sub-laplacianmentioning
confidence: 99%
“…For more details and explanations, we refer to [56]. Let U be a relatively compact open subset of a normal coordinate neighborhood ζ , as in Theorem 3.43.…”
Section: Definition 341mentioning
confidence: 99%
“…Our aim is to find suitable conditions on K which enable to prove the existence on M of a contact formθ C R conformal to θ , having the function K as Webster scalar curvature, Rθ = K . We writeθ = u 2 n θ, where u is a positive function defined on M. We obtain the following transformation law for the conformal Laplacians −L θ and −L θ , see [56].…”
Section: Preliminariesmentioning
confidence: 99%
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